14 Legendre and Related FunctionsReal Arguments

§14.8 Behavior at Singularities

Contents
  1. §14.8(i) x→1− or x→−1+
  2. §14.8(ii) x→1+
  3. §14.8(iii) x→∞

§14.8(i) x→1− or x→−1+

As x→1−,

14.8.1 𝖯νμ⁡(x) ∼1Γ⁡(1−μ)⁢(21−x)μ/2,
μ≠1,2,3,…,
14.8.2 𝖯νm⁡(x) ∼(−1)m⁢(ν−m+1)2⁢mm!⁢(1−x2)m/2,
m=1,2,3,…, ν≠m−1,m−2,…,−m,
14.8.3 𝖰ν⁡(x) =12⁢ln⁡(21−x)−γ−ψ⁡(ν+1)+O⁡((1−x)⁢ln⁡(1−x)),
ν≠−1,−2,−3,…,

where γ is Euler’s constant (§5.2(ii)). In the next three relations ℜ⁡μ>0.

14.8.4 𝖰νμ⁡(x)∼12⁢cos⁡(μ⁢π)⁢Γ⁡(μ)⁢(21−x)μ/2,
μ≠12,32,52,…,
14.8.5 𝖰νμ⁡(x)∼(−1)μ+(1/2)⁢π⁢Γ⁡(ν+μ+1)2⁢Γ⁡(μ+1)⁢Γ⁡(ν−μ+1)⁢(1−x2)μ/2,
μ=12,32,52,…, ν±μ≠−1,−2,−3,…,
14.8.6 𝖰ν−μ⁡(x)∼Γ⁡(μ)⁢Γ⁡(ν−μ+1)2⁢Γ⁡(ν+μ+1)⁢(21−x)μ/2,
ν±μ≠−1,−2,−3,….

The behavior of 𝖯νμ⁡(x) and 𝖰νμ⁡(x) as x→−1+ follows from the above results and the connection formulas (14.9.8) and (14.9.10).

§14.8(ii) x→1+

14.8.7 Pνμ⁡(x) ∼1Γ⁡(1−μ)⁢(2x−1)μ/2,
μ≠1,2,3,…,
14.8.8 Pνm⁡(x) ∼Γ⁡(ν+m+1)m!⁢Γ⁡(ν−m+1)⁢(x−12)m/2,
m=1,2,3,…, ν±m≠−1,−2,−3,…,
14.8.9 𝑸ν⁡(x) =−ln⁡(x−1)2⁢Γ⁡(ν+1)+12⁢ln⁡2−γ−ψ⁡(ν+1)Γ⁡(ν+1)+O⁡((x−1)⁢ln⁡(x−1)),
ν≠−1,−2,−3,…,
14.8.10 𝑸−n⁡(x)→(−1)n+1⁢(n−1)!,
n=1,2,3,…,
14.8.11 𝑸νμ⁡(x)∼Γ⁡(μ)2⁢Γ⁡(ν+μ+1)⁢(2x−1)μ/2,
ℜ⁡μ>0, ν+μ≠−1,−2,−3,….

§14.8(iii) x→∞

14.8.15 𝑸νμ⁡(x)∼π1/2Γ⁡(ν+32)⁢(2⁢x)ν+1,
ν≠−32,−52,−72,…,
14.8.16 𝑸−n−(1/2)μ⁡(x)∼π1/2⁢Γ⁡(μ+n+12)n!⁢Γ⁡(μ−n+12)⁢(2⁢x)n+(1/2),
n=1,2,3,…, μ−n+12≠0,−1,−2,….